Question #13515

A particle is moving along a line parallel to x-axis at a distance d from x-axis, with constant speed u. Find its radial acceleration using polar coordinates

Expert's answer


Suppose the particle has coordinates (R,ϕ)(R, \phi) at some moment tt. The formula for radial acceleration is:


a=v2Ra = \frac{v^2}{R}


where vv is a tangential velocity.

As vv is perpendicular to OB (because it is tangential velocity), we get from the scheme that:


v=usinϕv = u \sin \phi


Then


a(R,ϕ)=u2sin2ϕRa(R, \phi) = \frac{u^2 \sin^2 \phi}{R}


If we assume that at the moment t0=0t_0 = 0 the particle was at the point A (just in opposite to the origin), then it was at the point B at some moment tt and AB=utAB = ut.

Then we get:


R=u2t2+d2R = \sqrt{u^2 t^2 + d^2}


and


tanϕ=dut\tan \phi = \frac {d}{u t}


So, sin2ϕ=1cos2ϕ=111+tan2ϕ=tan2ϕ1+tan2ϕ=d2u2t2+d2.\sin^2\phi = 1 - \cos^2\phi = 1 - \frac{1}{1 + \tan^2\phi} = \frac{\tan^2\phi}{1 + \tan^2\phi} = \frac{d^2}{u^2t^2 + d^2}.

Finally,


a(t)=u2u2t2+d2d2u2t2+d2=u2d2(u2t2+d2)32a (t) = \frac {u ^ {2}}{\sqrt {u ^ {2} t ^ {2} + d ^ {2}}} * \frac {d ^ {2}}{u ^ {2} t ^ {2} + d ^ {2}} = \frac {u ^ {2} d ^ {2}}{(u ^ {2} t ^ {2} + d ^ {2}) ^ {\frac {3}{2}}}

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